Abstract
Most marine jet-propelled animals have low swimming efficiencies and relatively small jet orifices. Motivated by this, the present computational fluid dynamics study simulates the flow for a jet-propelled axisymmetric body swimming steadily at intermediate Reynolds numbers of order 1–1000. Results show that swimming-imposed flow field, drag coefficients, swimming efficiencies, and performance index (a metric comparing swimming speeds sustained by differently sized orifices ejecting the same volume flow rate) all depend strongly on orifice size, and orifice size affects the configuration of oppositely signed body vorticity and jet vorticity, thereby affecting wake and efficiency. As orifice size decreases, efficiencies decrease considerably, while performance index increases substantially, suggesting that, for a given jet volume flow rate, a smaller orifice supports faster swimming than a larger one does, albeit at reduced efficiency. These results support the notion that most jet-propelled animals having relatively small jet orifices may be an adaptation to deal with the physical constraint of limited total volume of water available for jetting, while needing to compete for fast swimming. Finally, jet orifice size is discussed regarding the role of jet propulsion in jet-propelled animal ecology, particularly for salps that use two relatively large siphons to respectively draw in and expel water.
Highlights
Quite a number of marine animals swim using jet propulsion, by which thrust is generated by ejecting water from an opening to attain body motion in the opposite direction [1,2]
Efficiency of animal jet propulsion is commonly quantified using the Froude propulsion efficiency (η FPE ), defined as the ratio of the useful power done against drag to the total jet power [1,2]
The present computational fluid dynamics (CFD) simulation study was directly motivated by the observationa that most marine study jet-propelled animals have low propulsionfact efficiencies
Summary
Quite a number of marine animals swim using jet propulsion, by which thrust is generated by ejecting water from an opening to attain body motion in the opposite direction [1,2]. They include squid [3,4,5,6,7,8], Nautilus [9,10,11], jellyfish [12,13,14,15,16], salps [17,18,19], etc. A time-resolved particle image velocimetry (PIV) method was used to measure the jet flow of the squid
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